The 63rd JSAP Spring Meeting, 2016

Presentation information

Poster presentation

15 Crystal Engineering » 15.5 Group IV crystals and alloys

[21p-P9-1~9] 15.5 Group IV crystals and alloys

Mon. Mar 21, 2016 1:30 PM - 3:30 PM P9 (Gymnasium)

1:30 PM - 3:30 PM

[21p-P9-6] Investigation of Σ3 Generation on Random Grain Boundary in Multicrystalline Silicon

〇(P)Xianjia Luo1, Jun Chen1, Takashi Sekiguchi1 (1.National Institute for Materials Science (NIMS))

Keywords:multicrystalline silicon,grain boundary,EBIC

Fundamental investigation of crystal growth in multicrystalline Si (mc-Si) is important in order to improve the crystal quality and device performance. However, Σ3 generation is unavoidable in crystal growth of mc-Si. Thus, it is necessary to understand the effect of Σ3 generation on device performance. In this work, we investigated the effect of Σ3 generation on random (R) grain boundaries (GBs) by means of electron-beam-induced current (EBIC) and electron-back-scatter diffractions (EBSD). The EBIC result indicates that Σ3 generation affects the electrical activity of R GBs at the initial stage of crystal growth, while does not impact on it at the steady stage. The reason of EBIC contrast variation of R GBs was studied. R GBs refer to large angle (LA) GBs except Σ3, Σ9 and 27. Fig. 1(a) shows that one LA grain boundary (GB) change to another LA GB after Σ3 generation and misorientation change between two LA GBs is about 7º. Fig. 1 (b) and (c) show that the EBIC contrast variation is large after Σ3 generation at the initial stage, while almost the same at the steady stage. High misorientation change had large EBIC contrast variation at the steady stage, whereas large EBIC contrast variation of high misorientation change was found at the initial stage. This result reveals that the structure of R GB is inclined to change after Σ3 generation at the initial stage. On the other hand, the structure of R GB tends to be stable after Σ3 generation at the steady stage. We also found that large EBIC contrast variation corresponded to high angle θ which was the angle between original R GB and new R GB after Σ3 generation. In conclusion, the structure of R GB is unstable at the initial stage and tends to change through Σ3 generation, which results in large EBIC contrast variation and high angle θ. High angle θ leads to high possibility of annihilation with other GB. After crystal growth to the steady stage, most of unstable R GB annihilated. Thus, at the steady stage Σ3 generation almost does not change the structure of R GB, namely its EBIC contrast.